Physics-based Modeling and Control of Homogeneous Charge Compression Ignition (HCCI) Engines - PowerPoint PPT Presentation

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Physics-based Modeling and Control of Homogeneous Charge Compression Ignition (HCCI) Engines

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Physics-based Modeling and Control of Homogeneous Charge Compression Ignition (HCCI) Engines Gregory M. Shaver Dynamic Design Lab May 6th, 2005 – PowerPoint PPT presentation

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Title: Physics-based Modeling and Control of Homogeneous Charge Compression Ignition (HCCI) Engines


1
Physics-based Modeling and Control of Homogeneous
Charge Compression Ignition (HCCI) Engines
  • Gregory M. Shaver
  • Dynamic Design Lab
  • May 6th, 2005
  • Department of Mechanical Engineering
  • Stanford University

2
Outline
  • What is residual-affected HCCI? What are its
    benefits?
  • Hurdles to practically implementing HCCI
  • Lack of combustion trigger
  • Cyclic coupling
  • Dynamic modeling of HCCI
  • Making HCCI practical with feedback control
  • Conclusions and future work

3
What is Residual-Affected HCCI?
  • Residual-Affected Homogeneous Charge Compression
    Ignition
  • Advanced combustion strategy for piston engines
  • Combustion due to uniform auto-ignition using
    compression alone
  • Hot exhaust gases reinducted using Variable Valve
    Actuation (VVA)
  • Main benefits
  • Increased efficiency compared to SI
  • Modest compression ratios
  • Drastic reduction in NOx emissions (i.e. smog)

4
HCCI with Variable Valve Actuation
5
HCCI with Variable Valve Actuation
  • Reactants (fuel air) previously exhausted
    gases (residual) inducted

6
HCCI with Variable Valve Actuation
  • Reactants (fuel air) previously exhausted
    gases (residual) inducted
  • Compression of mixture

7
HCCI with Variable Valve Actuation
  • Reactants (fuel air) previously exhausted
    gases (residual) inducted
  • Compression of mixture causes auto-ignition
  • uniform, fast uncontrolled

8
HCCI with Variable Valve Actuation
  • Reactants (fuel air) previously exhausted
    gases (residual) inducted
  • Compression of mixture causes auto-ignition
  • uniform, fast uncontrolled
  • Useful work from expansion

9
HCCI with Variable Valve Actuation
  • Reactants (fuel air) previously exhausted
    gases (residual) inducted
  • Compression of mixture causes auto-ignition
  • uniform, fast uncontrolled
  • Useful work from expansion
  • Hot combustion products exhausted

10
HCCI with Variable Valve Actuation
  • Reactants (fuel air) previously exhausted
    gases (residual) inducted
  • Compression of mixture causes auto-ignition
  • uniform, fast uncontrolled
  • Useful work from expansion
  • Hot combustion products exhausted, portion
    reinducted

11
HCCI with Variable Valve Actuation
  • Valve motions from VVA determine
  • inducted gas composition
  • amount of compression

12
HCCI with Variable Valve Actuation
13
HCCI with Variable Valve Actuation
  • Sudden rise in pressure combustion
    initiation

14
HCCI with Variable Valve Actuation
  • Sudden rise in pressure combustion
    initiation
  • Work output

15
HCCI with VVA -Challenges
  • Goal achieve desired combustion timing work
    output
  • Challenges
  • No direct initiator of combustion
  • Cycle-to-cycle coupling through exhaust gas
  • Significantly complicate transient load operation

16
HCCI with VVA -Challenges
  • Goal achieve desired combustion timing work
    output
  • Challenges
  • No direct initiator of combustion
  • Cycle-to-cycle coupling through exhaust gas
  • Significantly complicate transient load operation
  • To date HCCI impractical!!

17
Research Goals
  • Make HCCI practical through closed-loop control
  • Stabilize process control work output
  • Modeling Objective Simple physical models that
    capture behavior most relevant for control
  • Cyclic coupling
  • Combustion timing
  • In-cylinder pressure evolution (work output)
  • Control Objective - Control of
  • Combustion timing make combustion sure happens!
  • Work output the key output of the engine
  • efficiency reduced emissions come as result of
    process

18
Previous Work Simulation Modeling
  • Ogink and Golovitchev 2002, Babajimopoulos et al.
    2002
  • Multi-zone modeling of HCCI
  • Kong et al. 2002
  • Multi-dimensional CFD models using detailed
    chemistry
  • Many others
  • Complex flow and chemical kinetics models
  • Capture general steady state behavior
  • Ignore cycle-to-cycle coupling
  • Exhibit long run times - 12 hours per engine
    cycle

19
Contributions Simulation Modeling
  • Developed a simulation model of residual-affected
    HCCI that
  • Captures the cyclic coupling
  • Predicts behavior during steady state
    transients
  • Captures ignition via kinetics with a simple,
    intuitive model
  • runtimes 15 seconds per engine cycle (amenable
    to use as a control testbed)

20
Previous Work - Control
  • Agrell et al. 2003, Haraldsson et al. 2003,
    Bengtsson et al. 2004, Olsson et al. 2001,
    Matthews et al. 2005, others
  • Various approaches to control combustion timing
    or work output
  • In all cases controller hand-tuned or
    synthesized from black-box models

21
Contributions - Control
  • Physics-based control model of HCCI
  • The first physics-based approach to control of
    HCCI
  • Generalizable
  • Enables use of control engineering tools
  • Theoretical control design
  • Stability analysis
  • Control strategies for
  • Combustion timing
  • Peak pressure or work output

22
Outline - Modeling Strategies
  • Simulation model
  • Gain some intuition of the process
  • What are key features?
  • What are relevant control inputs outputs?
  • Control model
  • Need a slightly simpler physical description for
    synthesis
  • The launching point for developing control
    strategies
  • ..making HCCI practical!!

23
Experimental Apparatus
  • Single cylinder engine
  • With VVA
  • Fuel used Propane
  • Compression ratio
  • Variable 13-15.5
  • Engine speed
  • Fixed 1800 rpm
  • In-cylinder pressure transducer
  • Combustion timing
  • Peak pressure
  • Work output

24
HCCI Simulation Model
  • 1st law analysis of cylinder and exhaust manifold

25
HCCI Simulation Model
  • 1st law analysis of cylinder and exhaust manifold
  • Steady state 1D compressible flow relations

26
HCCI Simulation Model
  • 1st law analysis of cylinder and exhaust manifold
  • Steady state 1D compressible flow relations
  • Heat transfer
  • In-cylinder (modified Woschni)
  • Ref Chang et al. 2004
  • Exhaust manifold

27
HCCI Simulation Model
  • 1st law analysis of cylinder and exhaust manifold
  • Steady state 1D compressible flow relations
  • Heat transfer
  • In-cylinder (modified Woschni)
  • Ref Chang et al. 2004
  • Exhaust manifold
  • Combustion model
  • Wiebe function
  • What do we use as a combustion trigger?

28
HCCI Simulation Model
  • 1st law analysis of cylinder and exhaust manifold
  • Steady state 1D compressible flow relations
  • Heat transfer
  • In-cylinder (modified Woschni)
  • Ref Chang et al. 2004
  • Exhaust manifold
  • Combustion model
  • Wiebe function
  • What do we use as a combustion trigger?
  • Resulting Model 9 nonlinear ODEs

29
Temperature Threshold
  • Assume HCCI occurs at a threshold temperature
  • A fit at one temperature

30
Temperature Threshold
  • Assume HCCI occurs at a threshold temperature
  • Fit at one temperature doesnt hold at others!

Increasing residual
31
What Happened?
  • Simulation model earlier timing for increasing
    residual
  • More residual means mixture temperature
  • Higher temperature leads to early timing
  • Experiments show more constant timing
  • Is some physical effect missing?
  • Yes! Concentration of reactants
  • More residual means lower reactant concentration

32
Integrated Arrhenius Rate Equation
  • Simple model for start of combustion
  • Integrated Arrhenius rate
  • Constant threshold,
  • a, b and Ea from published experiments
  • Contributions from temperature reactant
    concentration captured

33
Integrated Arrhenius Rate
  • Set threshold at one operating point

34
Integrated Arrhenius Rate
  • Set threshold at one operating point and
    pressure, timing work output at all points is
    captured

Increasing residual
35
Integrated Arrhenius Rate
  • Note can vary composition without much change in
    timing

Increasing residual
36
Simulation Model Can it be extended?
  • Steady state behavior with propane captured
  • What about transients?
  • Changes in load
  • Can the model capture these?

37
Simulation Model Transients
  • 1st operating point has higher steady state
    temperature than 2nd
  • The elevated exhaust temperature advances
    combustion process during transition
  • As exhaust temperature decreases, behavior
    reaches new steady state

Experiment
38
Simulation Model Transients
Experiment
  • Simple model captures the coupling and ignition
    behavior during transition

Simulation
39
Results from Simulation modeling
  • Aspects most relevant for control captured with
    simple simulation model
  • Cyclic coupling combustion timing
  • In-cylinder pressure evolution
  • Approach can handle
  • Steady-state behavior
  • Transients
  • A valuable virtual testbed for control

40
Motivation for Control Model
  • Simulation model has a lot of benefits
  • Still, too complex for synthesizing control
    strategies
  • Motivates a simpler dynamic model
  • Enabled through additional physical assumptions
  • Discretizing the process (induction, compression,
    etc.)
  • Linking processes

41
Control Model Assumptions
  • Assumptions
  • Induction atmospheric pressure
  • Isentropic compression expansion
  • HCCI is fast constant volume combustion
  • In-cylinder heat transfer of combustion energy

42
Control Model Assumptions
43
A Simple Control Model
44
A Simple Control Model
  • Step through process to develop model of dynamics

45
A Simple Control Model
  • Step through process to develop model of dynamics

dynamics
46
Peak Pressure Dynamics
  • The peak pressure dynamics takes the form
  • Fairly complex nonlinear dynamic model

47
Peak Pressure Dynamics
  • The peak pressure dynamics takes the form
  • Fairly complex nonlinear dynamic model
  • Can see dependence on
  • Control inputs

48
Peak Pressure Dynamics
  • The peak pressure dynamics takes the form
  • Fairly complex nonlinear dynamic model
  • Can see dependence on
  • Control inputs
  • Cyclic coupling

49
Peak Pressure Dynamics
  • The peak pressure dynamics takes the form
  • Fairly complex nonlinear dynamic model
  • Can see dependence on
  • Control inputs
  • Cyclic coupling
  • Combustion timing

50
Peak Pressure Dynamics
  • The peak pressure dynamics takes the form
  • Fairly complex nonlinear dynamic model
  • Can see dependence on
  • Control inputs
  • Cyclic coupling
  • Combustion timing
  • How do we model initiation of combustion, qcomb?

51
Combustion Timing Dynamics
  • Recall the integrated Arrhenius rate model

52
Combustion Timing Dynamics
  • Recall the integrated Arrhenius rate model
  • Integrand takes on largest value at TDC

53
Combustion Timing Dynamics
  • Recall the integrated Arrhenius rate model
  • Integrand takes on largest value at TDC
  • Simplify begin integration at TDC with values at
    TDC

54
Combustion Timing Dynamics
  • Recall the integrated Arrhenius rate model
  • Integrand takes on largest value at TDC
  • Simplify begin integration at TDC with values at
    TDC

55
Combustion Timing Dynamics
  • Recall the integrated Arrhenius rate model
  • Integrand takes on largest value at TDC
  • Simplify begin integration at TDC with values at
    TDC

56
Combustion Timing Dynamics
  • Recall the integrated Arrhenius rate model
  • Integrand takes on largest value at TDC
  • Simplify begin integration at TDC with values at
    TDC
  • Algebraic expression exists for each variable

57
Combustion Timing Dynamics
  • Recall the integrated Arrhenius rate model
  • Integrand takes on largest value at TDC
  • Simplify begin integration at TDC with values at
    TDC
  • Algebraic expression exists for each variable

58
Control Model
  • Peak pressure and combustion timing dynamics
    together give
  • A nonlinear 2-state, dynamic, discrete system
    model

59
Control Model Validation
  • Control model captures
  • Steady state transient
  • Peak pressure
  • Combustion Timing
  • Captures
  • Cyclic coupling
  • Ignition via kinetics

60
Control Modeling Summary
  • HCCI is difficult to control
  • Cyclic coupling
  • No direct combustion trigger
  • Control model captures these phenomena!!
  • Simple model tells us how dynamics are affected
    by control inputs
  • Is a launching point for
  • Synthesizing control strategies
  • Assessing system stability
  • Generalizable

61
Outline of Control Implementations
  • From control model
  • Peak-pressure control at constant combustion
    timing
  • Work output control at constant combustion timing
  • Simultaneous peak pressure and combustion timing
    control
  • Many other approaches possible

62
Peak Pressure Control w/ Constant timing
  • Fix final valve closure
  • Vary composition to control peak pressure
  • A static approach to controlling timing
  • A large number of control approaches can be
    utilized

63
Peak Pressure Control w/ Constant timing Linear
Controller Synthesis
  • A common control approach is to linearize the
    system model
  • Linearizing about an operating point
    yields
  • Simple linear control laws can be synthesized

where
64
Peak Pressure Control w/ Constant timing
  • In closed-loop
  • Controller synthesized from linearized version of
    model
  • Is controller stable in closed-loop with
    nonlinear model?

65
Peak Pressure Control w/ Constant timing
Nonlinear Stability Analysis
  • Using
  • Lyapunov stability theory
  • Convex optimization
  • Shows
  • Simple linear controller stabilizes entire
    operating regime

66
Peak Pressure Control w/ Constant timing
Experimental Implementation
  • Accurate control of peak pressure
  • Mean tracking
  • Fluctuation reduction
  • Increases robustness
  • Little change in phase
  • What about direct control of work output (IMEP)?

67
Experimental Work Output Control
  • Rapid mean tracking fluctuation reduction
  • We can control work output, while keeping timing
    roughly constant

68
Experimental Work Output Control
  • Positive and negative load transients
  • What about simultaneous control of combustion
    timing and work output?

69
Combustion Timing Work Output Control
  • Add other control input final valve closure
  • Significant control knob for combustion timing
  • Simple approach
  • Separate linear controllers for peak pressure and
    timing

70
Decoupled Peak Pressure and Phase Control
  • Maintain cycle-to-cycle peak pressure controller,
    vary phase more slowly

71
Experiments with Decoupled Control
  • Approach works
  • Simultaneous control of
  • timing and peak pressure

72
Comments on Control Experiments
  • Simple physics-based controllers works well
  • Implementation is straightforward
  • Mean tracking fluctuation reduction of
  • peak pressure
  • work output
  • Combustion timing fairly constant
  • Independent control of peak pressure combustion
    timing
  • Many others possible

73
Conclusion
  • HCCI has a promising future as a cleaner, more
    efficient strategy
  • Hurdle controlling the process
  • No combustion initiator cycle-to-cycle coupling
  • The good news HCCI is amenable to model-based
    control
  • Key behaviors captured in both simulation and
    control models
  • Simulation control models capture
  • Steady-state
  • Transients
  • Physics-based control of
  • Peak pressure
  • Work output
  • Combustion timing

74
Future Work
  • Study different control approaches
  • Control of multi-cylinder HCCI engines
  • Results to date with single-cylinder engines
  • Cylinder-to-cylinder dynamics now play a key
    role!
  • Change the world!

75
Acknowledgments
  • Chris Gerdes
  • The Dynamic Design Lab
  • Partners in crime
  • Matt Roelle Nikhil Ravi
  • A great sponsor Robert Bosch Corporation
  • Jean-Pierre Hathout, Jasim Ahmed, Aleks Kojic
    Sungbae Park
  • The defense Committee
  • Chris Edwards, Sanjay Lall, Matt Franchek Steve
    Rock
  • Stanford University
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